Simulation of MA(1) Longitudinal Negative Binomial Counts and Using a Generalized Methods of Moment Equation Approach

Size: px
Start display at page:

Download "Simulation of MA(1) Longitudinal Negative Binomial Counts and Using a Generalized Methods of Moment Equation Approach"

Transcription

1 Chaot Modeln and Smulaton CMSM 3: Smulaton of MA Lontudnal Neatve Bnomal Counts and Usn a Genealzed Methods of Moment Equaton Appoah Naushad Mamode Khan epatment of Eonoms and StatstsUnvest of MautusRedut Mautus E-mal:n.mamodekhan@uom.a.mu Abstat Lontudnal ount data often ase n fnanal and medal studes. n suh applatons the data exhbt moe vaablt and thus the vaane to mean ato s eate than one. Unde suh umstanes the neatve bnomal s moe onvenent to be used fo modeln these lontudnal esponses. Sne these esponses ae olleted ove tme fo the same subjet t s moe lkel that the wll be oelated. n lteatue vaous oelaton models have been poposed and amon them the most popula ae the autoeessve and the movn aveae stutues. Besdes these esponses ae often subjet to multple ovaates that ma be tme-ndependent o tme-dependent. n the event of tme-ndependene t s elatvel eas to smulate and model the lontudnal neatve bnomal ounts follown the MA stutues but as fo the ase of tmedependene the smulaton of the MA lontudnal ount esponses s a hallenn poblem. n ths pape we wll use the bnomal thnnn opeaton to eneate sets of MA non-statona lontudnal neatve bnomal ounts and the effen of the smulaton esults ae assessed va a enealzed method of moments appoah. Kewods: Neatve Bnomal Lontudnal Movn Aveae Bnomal thnnn Statona Nonstatona Genealzed method of moments ntoduton n toda s ea lontudnal data has beome extemel useful n applatons elated to the health and fnanal setos. t onsttutes of a numbe of subjets that ae measued ove a spefed numbe of tme ponts. Sne these measuements ae olleted fo a patula subjet on a epettve bass t s moe lkel that the data wll be oelated. he oelaton stutues ma be follown autoeessve movn aveae equoelaton unstutued o an othe eneal autooelaton stutues45. Moeove n lontudnal studes the esponses ae nfluened b man fatos suh as n the analss of C4 ounts the nfluental fatos ae the teatment ae ende and man othes. n ode to estmate the ontbuton and the snfane of eah of these fatos Reeved: 8 Jul 04 / Aepted: 5 eembe CMSM SSN

2 36 Khan towads the esponse vaable t s mpotant to tansfom the data set-up nto a eesson famewok. n lteatue the eesson paametes have been estmated b vaous appoahes. ntall the method of Genealzed Estmatn equatons GEE wee developed but t fals unde msspefed oelaton stutue patulal unde the ndependene oelaton stutue 5. heeafte Pente and Zhao developed a Jont Estmaton appoah to estmate jontl the eesson and oelaton paametes and elded moe effent eesson estmates than the GEE appoah but the jont estmaton s based on hhe ode moments. he appoah s also based on the wokn oelaton stutue but the pesene of these hh ode moments dlute the msspefaton effet and boost the effen of the estmates. On the othe hand Qu and Lndsa 3 developed an adaptve quadat nfeene based Genealzed Method of Moments GMM appoah whee the assumed powes of the empal ovaane mates as the bases. hese bases ae then used to fom soe vetos o moment estmatn equatons and theeafte the wee ombned to fom a quadat funton n a smla wa as the GMM appoah. hs appoah of analzn lontudnal eesson models has so fa been tested on nomal Posson data 3 but has not et been exploed n neatve bnomal oelated ounts data. n ths pape ou objetves ae to develop the moment estmatn equatons based neatve bnomal model onstut the quadat nfeene funton and then obtan the eesson estmates b maxmzn the funton. Howeve one hallenn ssue s that sne the neatve bnomal model s a two paamete model that s dependn on the mean and ove-dspeson paamete t mples that we wll eque hhe ode moments. hs estmaton appoah wll be tested va smulatons on MA statona and non-statona neatve bnomal ounts. he oanzaton of the pape s as follows: n the next seton we wll evew the neatve bnomal model alon wth ts MA Gaussan autooelaton stutue and the adaptve GMM appoah follown Qu and Lndsa 3. n seton 3 we wll develop the estmatn equatons fo the neatve bnomal model followed b smulaton esults. Neatve Bnomal model Lontudnal data ompse of data that ae olleted epeatedl ove t 3 tme ponts fo subjets 3. hus an th andom obsevaton at t tme pont wll have a epesentaton of the fom t. he neatve bnomal model fo t s ven b t t f t t! t t E t exp x and a t 0 wth notaton fom t t t t t ~ NeBn t t th whee n

3 Chaot Modeln and Smulaton CMSM 3: ven a p veto of ovaates fom... p x t and veto of eesson paametes of the... t... and... t.... Sne these ounts t ae olleted epeatedl ove tme t s moe lkel that t wll be oelated ove tme. n ths pape we wll assume that the smulated t set of esponse vaables ome fom the faml of MA Gaussan autooelaton stutue. he devaton of the MA statona neatve bnomal ounts follows fom MKenze bnomal thnnn poess. Howeve the devaton of the MA non-statona oelaton stutue has not et appeaed n statstal lteatue. n the next seton we povde an n-depth devaton of the MA non-statona Gaussan autooelaton stutue. 3 MA Non-Statona Gaussan autooelaton Stutues n the non-statona set-up the mean paamete at eah tme pont wll dffe as the ovaates ae tme-dependent that t Follown MKenze we set up the famewok to eneate the MA non-statona Gaussan autooelaton stutue. the bnomal thnnn poess assumes that t d t t d t whee d NeBn t ~ t ~ Beta t t t = j pob b j t == t b z j t pob b =0=- t j t t and and hat s the ondtonal dstbuton of t d t follows the bnomal dstbuton wth paametes d t and t. Unde these assumptons t ~ NeBn t and the set of... t... t an be poved that follows the MA stutue.. Unde these dstbutonal assumptons we note that the ovaane

4 38 Khan between t and t k s ven b las the ovaane does not exst. tk tk fo k and fo othe 4. Smulaton of MA Non Statona NB ounts he smulaton poess wll follow fom the bnomal thnnn opeaton explaned n the pevous seton wth t exp x t that s we need to povde a ven set of ovaate desns and a set of eesson veto that espets the dmenson of the ovaate matx. Note that fo the statona ase the ovaate matx wll be tme ndependent whle fo the non-statona the ovaate desn wll be tme-dependent. As suh we assume fo the non-statona ase the follown desns esn A esn B esn C x t 0.5t bnom30. t t pos t t t... 4 x t x t 0.5t sn t t exp t t ost t... 4 t t ln t t t t... 4 and xt s eneated fom the Posson dstbuton wth mean paamete. n ths wa the mean paamete fo eah subjet wll va. hus fo these set of ovaates and ntal estmate of the eesson veto dspeson paamete and oelaton paamete we eneate MA Neatve Bnomal andom vaables b fst smulatn the eo

5 Chaot Modeln and Smulaton CMSM 3: omponents t d t and the thnnn opeaton andom vaables t t. Fo ou smulaton poess we wll assume the values of. 5. Estmaton Methodolo Qu and Lndsa 3 have developed an estmaton appoah based Genealzed Methods of Moments that do not eque an assumpton n the undeln oelaton stutue and do not eque an estmaton of the oelaton paamete. n fat Qu and Lnsda 3 assumed a soe veto that onl needs the empal ovaane estmaton matx whee s the adent matx: t t and s an othoonal veto. he alulaton of the paamete eques the onjuate adent method see Qu and Lndsa 3. n the ontext of the neatve bnomal model the soe veto s defned as: f f whee the vetos f f E f f and t whee t t 0 Usn the soe veto Qu and Lndsa 3 defned the objetve funton C Q

6 40 Khan whee C s the sample vaane of 3 B maxmzn the objetve funton wth espet to the unknown set of paametes we obtan the estmatn equaton Q wth. Sne the above estmatn equaton s non-lnea we solve the equaton usn the Newton-Raphson poedue that elds an teatve equaton of the fom ˆ ˆ ˆ ˆ Q Q C Q whee C s the double devatve hessan pat of the soe funton and ths s ben used fo alulatn the vaane of the eesson and ovedspeson paametes. As llustated b Qu and Lndsa 3 ths method elds onsstent and effent estmatos and tends towads asmptot nomalt fo lae sample sze. 6. Results and Conluson Follown the pevous setons we have un 0000 smulatons fo eah of the sample based on the dffeent ovaate desns fo the non- szes 500 statona set-ups. Note that fo the statona ase the mean s held onstant at all tme ponts whlst fo non-statona the mean vaes wth the tme ponts ven the tmedependent ovaates. he table povdes the smulated mean estmates of the eesson paametes alon wth the standad eos n bakets. esn A esn B esn C ; ;0.0.0; ; ; ; ; ; ; ; ; ; ; ;0.0.00; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ;0.076 Based on the smulaton esults we note that the estmates of the eesson paametes ae lose to the populaton values and as the sample sze neases the standad eos of the eesson paametes deease whh ndates that the estmates ae onsstent and

7 Chaot Modeln and Smulaton CMSM 3: effent. Howeve we have emaked a snfant numbe of falues n the smulatons as we nease the sample sze. hese falues wee manl due to ll-ondtoned natue of the double devatve Hessan matx. o oveome ths poblem n some smulatons we have used the Mooe Penose enealzed nvese method n R nv n Lba MASS to pefom the teatve poedues. Oveall the enealzed method of moments estmaton tehnque s a statstall sound tehnque but n tems of omputaton t ma not alwas be elable. Refeenes. E. MKenze. Autoeessve movn-aveae poesses wth neatve bnomal and eomet manal dstbutons. Advaned Appled Pobablt R. Pente R. & L. Zhao 99. Estmatn equatons fo paametes n means and ovaanes of multvaate dsete and ontnuous esponses. Bomets A.Qu & B. Lndsa 003. Buldn adaptve estmatn equatons when nvese of ovaane estmaton s dffult. Jounal of Roal Statstal Soet B. Sutadha. An ovevew on eesson models fo dsete lontudnal esponses. Statstal Sene B. Sutadha B. & K. as. On the effen of eesson estmatos n enealzed lnea models fo lontudnal data. Bometka

Multistage Median Ranked Set Sampling for Estimating the Population Median

Multistage Median Ranked Set Sampling for Estimating the Population Median Jounal of Mathematcs and Statstcs 3 (: 58-64 007 ISSN 549-3644 007 Scence Publcatons Multstage Medan Ranked Set Samplng fo Estmatng the Populaton Medan Abdul Azz Jeman Ame Al-Oma and Kamaulzaman Ibahm

More information

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions A Bef Gude to Recognzng and Copng Wth Falues of the Classcal Regesson Assumptons Model: Y 1 k X 1 X fxed n epeated samples IID 0, I. Specfcaton Poblems A. Unnecessay explanatoy vaables 1. OLS s no longe

More information

Clustering Techniques

Clustering Techniques Clusteng Tehnques Refeenes: Beln Chen 2003. Moden Infomaton Reteval, haptes 5, 7 2. Foundatons of Statstal Natual Language Poessng, Chapte 4 Clusteng Plae smla obets n the same goup and assgn dssmla obets

More information

Set of square-integrable function 2 L : function space F

Set of square-integrable function 2 L : function space F Set of squae-ntegable functon L : functon space F Motvaton: In ou pevous dscussons we have seen that fo fee patcles wave equatons (Helmholt o Schödnge) can be expessed n tems of egenvalue equatons. H E,

More information

A NOTE ON ELASTICITY ESTIMATION OF CENSORED DEMAND

A NOTE ON ELASTICITY ESTIMATION OF CENSORED DEMAND Octobe 003 B 003-09 A NOT ON ASTICITY STIATION OF CNSOD DAND Dansheng Dong an Hay. Kase Conell nvesty Depatment of Apple conomcs an anagement College of Agcultue an fe Scences Conell nvesty Ithaca New

More information

Special Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k.

Special Relativity in Acoustic and Electromagnetic Waves Without Phase Invariance and Lorentz Transformations 1. Introduction n k. Speial Relativit in Aousti and Eletomagneti Waves Without Phase Invaiane and Loentz Tansfomations Benhad Rothenstein bothenstein@gmail.om Abstat. Tansfomation equations fo the phsial quantities intodued

More information

New Bivariate Exponentiated Modified Weibull Distribution

New Bivariate Exponentiated Modified Weibull Distribution Jounal of Matheats and Statsts Ognal Reseah Pape New Bvaate Exponentated Modfed Webull Dstbuton Abdelfattah Mustafa and Mohaed AW Mahoud Depatent of Matheats, Fault of Sene, Mansoua Unvest, Mansoua 556,

More information

Efficiency of the principal component Liu-type estimator in logistic

Efficiency of the principal component Liu-type estimator in logistic Effcency of the pncpal component Lu-type estmato n logstc egesson model Jbo Wu and Yasn Asa 2 School of Mathematcs and Fnance, Chongqng Unvesty of Ats and Scences, Chongqng, Chna 2 Depatment of Mathematcs-Compute

More information

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time Intenatonal Jounal of ompute Applcatons (5 ) Volume 44 No, Apl Optmal System fo Wam Standby omponents n the esence of Standby Swtchng Falues, Two Types of Falues and Geneal Repa Tme Mohamed Salah EL-Shebeny

More information

Tutorial Chemical Reaction Engineering:

Tutorial Chemical Reaction Engineering: Dpl.-Ing. ndeas Jöke Tutoal Chemal eaton Engneeng:. eal eatos, esdene tme dstbuton and seletvty / yeld fo eaton netwoks Insttute of Poess Engneeng, G5-7, andeas.joeke@ovgu.de 8-Jun-6 Tutoal CE: esdene

More information

Research on Probability Density Estimation Method for Random Dynamic Systems

Research on Probability Density Estimation Method for Random Dynamic Systems 73 A publaton of VOL. 5, 6 CHEMICAL ENGINEERING TRANSACTIONS Guest Edtos: Thun Wang, Hongyang Zhang, Le Tan Copyght 6, AIDIC Sevz S..l., ISBN 978-88-9568-43-3; ISSN 83-96 The Italan Assoaton of Chemal

More information

Clustering. Outline. Supervised vs. Unsupervised Learning. Clustering. Clustering Example. Applications of Clustering

Clustering. Outline. Supervised vs. Unsupervised Learning. Clustering. Clustering Example. Applications of Clustering Clusteng CS478 Mahne Leanng Spng 008 Thosten Joahms Conell Unvesty Outlne Supevsed vs. Unsupevsed Leanng Heahal Clusteng Heahal Agglomeatve Clusteng (HAC) Non-Heahal Clusteng K-means EM-Algothm Readng:

More information

UNIT10 PLANE OF REGRESSION

UNIT10 PLANE OF REGRESSION UIT0 PLAE OF REGRESSIO Plane of Regesson Stuctue 0. Intoducton Ojectves 0. Yule s otaton 0. Plane of Regesson fo thee Vaales 0.4 Popetes of Resduals 0.5 Vaance of the Resduals 0.6 Summay 0.7 Solutons /

More information

Part V: Velocity and Acceleration Analysis of Mechanisms

Part V: Velocity and Acceleration Analysis of Mechanisms Pat V: Velocty an Acceleaton Analyss of Mechansms Ths secton wll evew the most common an cuently pactce methos fo completng the knematcs analyss of mechansms; escbng moton though velocty an acceleaton.

More information

Groupoid and Topological Quotient Group

Groupoid and Topological Quotient Group lobal Jounal of Pue and Appled Mathematcs SSN 0973-768 Volume 3 Numbe 7 07 pp 373-39 Reseach nda Publcatons http://wwwpublcatoncom oupod and Topolocal Quotent oup Mohammad Qasm Manna Depatment of Mathematcs

More information

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution oden Appled Scence The Fomn Theoy and the NC achnn fo The Rotay us wth the Spectal Ede Dstbuton Huan Lu Depatment of echancal Enneen, Zhejan Unvesty of Scence and Technoloy Hanzhou, c.y. chan, 310023,

More information

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15,

Event Shape Update. T. Doyle S. Hanlon I. Skillicorn. A. Everett A. Savin. Event Shapes, A. Everett, U. Wisconsin ZEUS Meeting, October 15, Event Shape Update A. Eveett A. Savn T. Doyle S. Hanlon I. Skllcon Event Shapes, A. Eveett, U. Wsconsn ZEUS Meetng, Octobe 15, 2003-1 Outlne Pogess of Event Shapes n DIS Smla to publshed pape: Powe Coecton

More information

ucta SS"7CIVIL ENGINEERING STUDIES

ucta SS7CIVIL ENGINEERING STUDIES 0 uta SS"7VL ENGNEERNG STUDES Stutual Reseah Sees No. 557 ULU-ENG-90-205 'SSN: 0069-4274 PARAMETER ESTMATON N OMPLEX LNEAR STRUTURES By Keth D. Helmstad Shaon L. Wood and Stephen. lak A epot on eseah sponsoed

More information

Chapter Fifiteen. Surfaces Revisited

Chapter Fifiteen. Surfaces Revisited Chapte Ffteen ufaces Revsted 15.1 Vecto Descpton of ufaces We look now at the vey specal case of functons : D R 3, whee D R s a nce subset of the plane. We suppose s a nce functon. As the pont ( s, t)

More information

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. Flux: = da i. Force: = -Â g a ik k = X i. Â J i X i (7. Themodynamcs and Knetcs of Solds 71 V. Pncples of Ievesble Themodynamcs 5. Onsage s Teatment s = S - S 0 = s( a 1, a 2,...) a n = A g - A n (7.6) Equlbum themodynamcs detemnes the paametes of an equlbum

More information

Lecture 4: Non linear parameter estimation problems: tools for enhancing metrological objectives

Lecture 4: Non linear parameter estimation problems: tools for enhancing metrological objectives Mett 5 Spng Shool Rosoff June 3-8, Letue 4: Non lnea paamete estmaton poblems: tools fo enhanng metologal objetves B. Rémy, S. Andé, D.Mallet LEMA, Unvesté de Loane & CNRS, Vandœuve-lès-Nany, Fane E-mal:

More information

Learning the structure of Bayesian belief networks

Learning the structure of Bayesian belief networks Lectue 17 Leanng the stuctue of Bayesan belef netwoks Mlos Hauskecht mlos@cs.ptt.edu 5329 Sennott Squae Leanng of BBN Leanng. Leanng of paametes of condtonal pobabltes Leanng of the netwok stuctue Vaables:

More information

Detection and Estimation Theory

Detection and Estimation Theory ESE 54 Detecton and Etmaton Theoy Joeph A. O Sullvan Samuel C. Sach Pofeo Electonc Sytem and Sgnal Reeach Laboatoy Electcal and Sytem Engneeng Wahngton Unvety 411 Jolley Hall 314-935-4173 (Lnda anwe) jao@wutl.edu

More information

3. A Review of Some Existing AW (BT, CT) Algorithms

3. A Review of Some Existing AW (BT, CT) Algorithms 3. A Revew of Some Exstng AW (BT, CT) Algothms In ths secton, some typcal ant-wndp algothms wll be descbed. As the soltons fo bmpless and condtoned tansfe ae smla to those fo ant-wndp, the pesented algothms

More information

COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE

COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE COMPARING MORE THAN TWO POPULATION MEANS: AN ANALYSIS OF VARIANCE To see how the piniple behind the analysis of vaiane method woks, let us onside the following simple expeiment. The means ( 1 and ) of

More information

Computation of Low-Frequency Electric Fields in Analysis of Electromagnetic Field Exposure

Computation of Low-Frequency Electric Fields in Analysis of Electromagnetic Field Exposure Computaton of Low-Fequeny Eet Feds n Anayss of Eetomagnet Fed Exposue Žejo Šth, Bojan Tuja, Sead Bebeovć Fauty of Eeta Engneeng and Computng Unvesty of Zageb Unsa 3, Zageb, Coata phone:+385 69 865, fax:

More information

P 365. r r r )...(1 365

P 365. r r r )...(1 365 SCIENCE WORLD JOURNAL VOL (NO4) 008 www.scecncewoldounal.og ISSN 597-64 SHORT COMMUNICATION ANALYSING THE APPROXIMATION MODEL TO BIRTHDAY PROBLEM *CHOJI, D.N. & DEME, A.C. Depatment of Mathematcs Unvesty

More information

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1 Rotatonal Knematcs Rgd Object about a Fxed Axs Westen HS AP Physcs 1 Leanng Objectes What we know Unfom Ccula Moton q s Centpetal Acceleaton : Centpetal Foce: Non-unfom a F c c m F F F t m ma t What we

More information

Physics 201 Lecture 4

Physics 201 Lecture 4 Phscs 1 Lectue 4 ltoda: hapte 3 Lectue 4 v Intoduce scalas and vectos v Peom basc vecto aleba (addton and subtacton) v Inteconvet between atesan & Pola coodnates Stat n nteestn 1D moton poblem: ace 9.8

More information

Advanced Topics of Artificial Intelligence

Advanced Topics of Artificial Intelligence Adaned Tops of Atfal Intellgene - Intoduton and Motaton - Tehnshe Unestät Gaz Unestät Klagenfut Motatng Eample to put the at befoe the hose 2 Motaton the ths yeas letue has two majo goals. to show moe

More information

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation Wold Academy of Scence, Engneeng and Technology 6 7 On Maneuveng Taget Tacng wth Onlne Obseved Coloed Glnt Nose Paamete Estmaton M. A. Masnad-Sha, and S. A. Banan Abstact In ths pape a compehensve algothm

More information

QUANTILE ESTIMATION: A MINIMALIST APPROACH

QUANTILE ESTIMATION: A MINIMALIST APPROACH Poeedngs o the 2006 Wnte Smulaton Coneene L. F. Peone F. P. Weland J. Lu B. G. Lawson D.. Nol and R.. Fujmoto eds QUANTILE ESTIATION: A INIALIST APPROACH Yuy Baksh AT&T Laboatoes 200 S Lauel Ave ddletown

More information

Vibration Input Identification using Dynamic Strain Measurement

Vibration Input Identification using Dynamic Strain Measurement Vbaton Input Identfcaton usng Dynamc Stan Measuement Takum ITOFUJI 1 ;TakuyaYOSHIMURA ; 1, Tokyo Metopoltan Unvesty, Japan ABSTRACT Tansfe Path Analyss (TPA) has been conducted n ode to mpove the nose

More information

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Physics 2A Chapter 11 - Universal Gravitation Fall 2017 Physcs A Chapte - Unvesal Gavtaton Fall 07 hese notes ae ve pages. A quck summay: he text boxes n the notes contan the esults that wll compse the toolbox o Chapte. hee ae thee sectons: the law o gavtaton,

More information

Photographing a time interval

Photographing a time interval Potogaping a time inteval Benad Rotenstein and Ioan Damian Politennia Univesity of imisoaa Depatment of Pysis imisoaa Romania benad_otenstein@yaoo.om ijdamian@yaoo.om Abstat A metod of measuing time intevals

More information

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law Physcs 11b Lectue # Electc Feld Electc Flux Gauss s Law What We Dd Last Tme Electc chage = How object esponds to electc foce Comes n postve and negatve flavos Conseved Electc foce Coulomb s Law F Same

More information

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1

Machine Learning. Spectral Clustering. Lecture 23, April 14, Reading: Eric Xing 1 Machne Leanng -7/5 7/5-78, 78, Spng 8 Spectal Clusteng Ec Xng Lectue 3, pl 4, 8 Readng: Ec Xng Data Clusteng wo dffeent ctea Compactness, e.g., k-means, mxtue models Connectvty, e.g., spectal clusteng

More information

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints. Mathematcal Foundatons -1- Constaned Optmzaton Constaned Optmzaton Ma{ f ( ) X} whee X {, h ( ), 1,, m} Necessay condtons fo to be a soluton to ths mamzaton poblem Mathematcally, f ag Ma{ f ( ) X}, then

More information

Dirichlet Mixture Priors: Inference and Adjustment

Dirichlet Mixture Priors: Inference and Adjustment Dchlet Mxtue Pos: Infeence and Adustment Xugang Ye (Wokng wth Stephen Altschul and Y Kuo Yu) Natonal Cante fo Botechnology Infomaton Motvaton Real-wold obects Independent obsevatons Categocal data () (2)

More information

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M Dola Bagayoko (0) Integal Vecto Opeatons and elated Theoems Applcatons n Mechancs and E&M Ι Basc Defnton Please efe to you calculus evewed below. Ι, ΙΙ, andιιι notes and textbooks fo detals on the concepts

More information

An Approach to Inverse Fuzzy Arithmetic

An Approach to Inverse Fuzzy Arithmetic An Appoach to Invese Fuzzy Athmetc Mchael Hanss Insttute A of Mechancs, Unvesty of Stuttgat Stuttgat, Gemany mhanss@mechaun-stuttgatde Abstact A novel appoach of nvese fuzzy athmetc s ntoduced to successfully

More information

Folding to Curved Surfaces: A Generalized Design Method and Mechanics of Origami-based Cylindrical Structures

Folding to Curved Surfaces: A Generalized Design Method and Mechanics of Origami-based Cylindrical Structures Supplementay Infomaton fo Foldng to Cuved Sufaes: A Genealzed Desgn Method and Mehans of Ogam-based Cylndal Stutues Fe Wang, Haoan Gong, X Chen, Changqng Chen, Depatment of Engneeng Mehans, Cente fo Nano/Mo

More information

Controller Design for Networked Control Systems in Multiple-packet Transmission with Random Delays

Controller Design for Networked Control Systems in Multiple-packet Transmission with Random Delays Appled Mehans and Materals Onlne: 03-0- ISSN: 66-748, Vols. 78-80, pp 60-604 do:0.408/www.sentf.net/amm.78-80.60 03 rans eh Publatons, Swtzerland H Controller Desgn for Networed Control Systems n Multple-paet

More information

8 Baire Category Theorem and Uniform Boundedness

8 Baire Category Theorem and Uniform Boundedness 8 Bae Categoy Theoem and Unfom Boundedness Pncple 8.1 Bae s Categoy Theoem Valdty of many esults n analyss depends on the completeness popety. Ths popety addesses the nadequacy of the system of atonal

More information

Scalars and Vectors Scalar

Scalars and Vectors Scalar Scalas and ectos Scala A phscal quantt that s completel chaacteed b a eal numbe (o b ts numecal value) s called a scala. In othe wods a scala possesses onl a magntude. Mass denst volume tempeatue tme eneg

More information

GENERALIZED MULTIVARIATE EXPONENTIAL TYPE (GMET) ESTIMATOR USING MULTI-AUXILIARY INFORMATION UNDER TWO-PHASE SAMPLING

GENERALIZED MULTIVARIATE EXPONENTIAL TYPE (GMET) ESTIMATOR USING MULTI-AUXILIARY INFORMATION UNDER TWO-PHASE SAMPLING Pak. J. Statst. 08 Vol. (), 9-6 GENERALIZED MULTIVARIATE EXPONENTIAL TYPE (GMET) ESTIMATOR USING MULTI-AUXILIARY INFORMATION UNDER TWO-PHASE SAMPLING Ayesha Ayaz, Zahoo Ahmad, Aam Sanaullah and Muhammad

More information

PHY126 Summer Session I, 2008

PHY126 Summer Session I, 2008 PHY6 Summe Sesson I, 8 Most of nfomaton s avalable at: http://nngoup.phscs.sunsb.edu/~chak/phy6-8 ncludng the sllabus and lectue sldes. Read sllabus and watch fo mpotant announcements. Homewok assgnment

More information

CHAPTER 10: LINEAR DISCRIMINATION

CHAPTER 10: LINEAR DISCRIMINATION HAPER : LINEAR DISRIMINAION Dscmnan-based lassfcaon 3 In classfcaon h K classes ( k ) We defned dsmnan funcon g () = K hen gven an es eample e chose (pedced) s class label as f g () as he mamum among g

More information

Single-Carrier Frequency Domain Adaptive Antenna Array for Distributed Antenna Network

Single-Carrier Frequency Domain Adaptive Antenna Array for Distributed Antenna Network Sngle-Cae Fequeny Doman Aaptve Antenna Aay fo Dstbute Antenna etwok We Peng Depatment of Eletal an Communaton ohoku Unvesty Sena, Japan peng@moble.ee.tohoku.a.jp Fumyuk Aah Depatment of Eletal an Communaton

More information

an application to HRQoL

an application to HRQoL AlmaMate Studoum Unvesty of Bologna A flexle IRT Model fo health questonnae: an applcaton to HRQoL Seena Boccol Gula Cavn Depatment of Statstcal Scence, Unvesty of Bologna 9 th Intenatonal Confeence on

More information

Computational Vision. Camera Calibration

Computational Vision. Camera Calibration Comutatonal Vson Camea Calbaton uo hate 6 Camea Calbaton Poblem: Estmate amea s etns & ntns aametes MthdU Method: Use mage(s) () o knon sene ools: Geomet amea models SVD and onstaned least-squaes Lne etaton

More information

However, this strict exogeneity assumption is rather strong. Consider the following model:

However, this strict exogeneity assumption is rather strong. Consider the following model: Dnamc Panel Data L Gan Septembe 00 The classc panel data settng assumes the stct eogenet: ( t,, T ( t t t + c Once t and c ae contolled fo, s has no patal effect on t fo s t. In ths case, t s stctl eogenous,

More information

Contact, information, consultations

Contact, information, consultations ontact, nfomaton, consultatons hemsty A Bldg; oom 07 phone: 058-347-769 cellula: 664 66 97 E-mal: wojtek_c@pg.gda.pl Offce hous: Fday, 9-0 a.m. A quote of the week (o camel of the week): hee s no expedence

More information

Introduction to Algorithms 6.046J/18.401J

Introduction to Algorithms 6.046J/18.401J 3/4/28 Intoduton to Algothms 6.46J/8.4J Letue 8 - Hashng Pof. Manols Kells Hashng letue outlne Into and defnton Hashng n pate Unvesal hashng Pefet hashng Open Addessng (optonal) 3/4/28 L8.2 Data Stutues

More information

Continuous-Time Bilinear System Identification

Continuous-Time Bilinear System Identification NASA/TM-2003-22646 Contnuous-Tme Blnea System Identfaton Je-Nan Juang Langley Reseah Cente, Hampton, Vgna Septembe 2003 The NASA STI Pogam Offe... n Pofle Sne ts foundng, NASA has been dedated to the advanement

More information

APPLICATIONS OF SEMIGENERALIZED -CLOSED SETS

APPLICATIONS OF SEMIGENERALIZED -CLOSED SETS Intenatonal Jounal of Mathematcal Engneeng Scence ISSN : 22776982 Volume Issue 4 (Apl 202) http://www.mes.com/ https://stes.google.com/ste/mesounal/ APPLICATIONS OF SEMIGENERALIZED CLOSED SETS G.SHANMUGAM,

More information

Correlation and Regression without Sums of Squares. (Kendall's Tau) Rudy A. Gideon ABSTRACT

Correlation and Regression without Sums of Squares. (Kendall's Tau) Rudy A. Gideon ABSTRACT Correlaton and Regson wthout Sums of Squa (Kendall's Tau) Rud A. Gdeon ABSTRACT Ths short pee provdes an ntroduton to the use of Kendall's τ n orrelaton and smple lnear regson. The error estmate also uses

More information

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model

6. Introduction to Transistor Amplifiers: Concepts and Small-Signal Model 6. ntoucton to anssto mples: oncepts an Small-Sgnal Moel Lectue notes: Sec. 5 Sea & Smth 6 th E: Sec. 5.4, 5.6 & 6.3-6.4 Sea & Smth 5 th E: Sec. 4.4, 4.6 & 5.3-5.4 EE 65, Wnte203, F. Najmaba Founaton o

More information

Experiment 1 Electric field and electric potential

Experiment 1 Electric field and electric potential Expeiment 1 Eleti field and eleti potential Pupose Map eleti equipotential lines and eleti field lines fo two-dimensional hage onfiguations. Equipment Thee sheets of ondutive papes with ondutive-ink eletodes,

More information

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation By Rudy A. Gdeon The Unvesty of Montana The Geatest Devaton Coelaton Coeffcent and ts Geometcal Intepetaton The Geatest Devaton Coelaton Coeffcent (GDCC) was ntoduced by Gdeon and Hollste (987). The GDCC

More information

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles /4/04 Chapte 7 Lnea oentu Lnea oentu of a Sngle Patcle Lnea oentu: p υ It s a easue of the patcle s oton It s a vecto, sla to the veloct p υ p υ p υ z z p It also depends on the ass of the object, sla

More information

Generating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences

Generating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences Geneatng Functons, Weghted and Non-Weghted Sums fo Powes of Second-Ode Recuence Sequences Pantelmon Stăncă Aubun Unvesty Montgomey, Depatment of Mathematcs Montgomey, AL 3614-403, USA e-mal: stanca@studel.aum.edu

More information

Diffraction from Crystals Shape Factor

Diffraction from Crystals Shape Factor Letue 3 Diffation fom Cystals Shape Fato - Fultz & Howe, Chap. 5 - Williams & Cate, Chap. 7 - Reime, Chap. 7 Satteed wave: Shape Fato Cystal size effet k F k ep i k Shape fato: S k ep ik z Unit ell (/w

More information

High Performance VLSI Architecture of 2D Discrete Wavelet Transform with Scalable Lattice Structure

High Performance VLSI Architecture of 2D Discrete Wavelet Transform with Scalable Lattice Structure Wold Aadem of Sene, Engneeng and Tehnolog Intenatonal Jounal of Eletons and Communaton Engneeng Hgh Pefomane VLSI Ahtetue of 2D Dsete Wavelet Tansfom wth Salable Latte Stutue Juoung Km, Taegeun Pa Intenatonal

More information

DOAEstimationforCoherentSourcesinBeamspace UsingSpatialSmoothing

DOAEstimationforCoherentSourcesinBeamspace UsingSpatialSmoothing DOAEstmatonorCoherentSouresneamspae UsngSpatalSmoothng YnYang,ChunruWan,ChaoSun,QngWang ShooloEletralandEletronEngneerng NanangehnologalUnverst,Sngapore,639798 InsttuteoAoustEngneerng NorthwesternPoltehnalUnverst,X

More information

PARAMETER ESTIMATION FOR TWO WEIBULL POPULATIONS UNDER JOINT TYPE II CENSORED SCHEME

PARAMETER ESTIMATION FOR TWO WEIBULL POPULATIONS UNDER JOINT TYPE II CENSORED SCHEME Sept 04 Vol 5 No 04 Intenatonal Jounal of Engneeng Appled Scences 0-04 EAAS & ARF All ghts eseed wwweaas-ounalog ISSN305-869 PARAMETER ESTIMATION FOR TWO WEIBULL POPULATIONS UNDER JOINT TYPE II CENSORED

More information

Parameter Estimation Method in Ridge Regression

Parameter Estimation Method in Ridge Regression Paamete Estmaton Method n dge egesson Dougade.V. Det. of tatstcs, hvaj Unvesty Kolhau-46004. nda. adougade@edff.com Kashd D.N. Det. of tatstcs, hvaj Unvesty Kolhau-46004. nda. dnkashd_n@yahoo.com bstact

More information

Confidence Intervals for the Squared Multiple Semipartial Correlation Coefficient. James Algina. University of Florida. H. J.

Confidence Intervals for the Squared Multiple Semipartial Correlation Coefficient. James Algina. University of Florida. H. J. Eet Size Conidene Inteval 1 Conidene Intevals o the Squaed Multiple Semipatial Coelation Coeiient by James Algina Univesity o Floida H. J. Keselman Univesity o Manitoba all D. Penield Univesity o Miami

More information

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41.

Chapter I Matrices, Vectors, & Vector Calculus 1-1, 1-9, 1-10, 1-11, 1-17, 1-18, 1-25, 1-27, 1-36, 1-37, 1-41. Chapte I Matces, Vectos, & Vecto Calculus -, -9, -0, -, -7, -8, -5, -7, -36, -37, -4. . Concept of a Scala Consde the aa of patcles shown n the fgue. he mass of the patcle at (,) can be epessed as. M (,

More information

N = N t ; t 0. N is the number of claims paid by the

N = N t ; t 0. N is the number of claims paid by the Iulan MICEA, Ph Mhaela COVIG, Ph Canddate epatment of Mathematcs The Buchaest Academy of Economc Studes an CECHIN-CISTA Uncedt Tac Bank, Lugoj SOME APPOXIMATIONS USE IN THE ISK POCESS OF INSUANCE COMPANY

More information

GLE 594: An introduction to applied geophysics

GLE 594: An introduction to applied geophysics GLE 594: An intoduction to applied geophsics Electical Resistivit Methods Fall 4 Theo and Measuements Reading: Toda: -3 Net Lectue: 3-5 Two Cuent Electodes: Souce and Sink Wh un an electode to infinit

More information

EE 5337 Computational Electromagnetics (CEM)

EE 5337 Computational Electromagnetics (CEM) 7//28 Instucto D. Raymond Rumpf (95) 747 6958 cumpf@utep.edu EE 5337 Computatonal Electomagnetcs (CEM) Lectue #6 TMM Extas Lectue 6These notes may contan copyghted mateal obtaned unde fa use ules. Dstbuton

More information

4 Recursive Linear Predictor

4 Recursive Linear Predictor 4 Recusve Lnea Pedcto The man objectve of ths chapte s to desgn a lnea pedcto wthout havng a po knowledge about the coelaton popetes of the nput sgnal. In the conventonal lnea pedcto the known coelaton

More information

OBSTACLE DETECTION USING RING BEAM SYSTEM

OBSTACLE DETECTION USING RING BEAM SYSTEM OBSTACLE DETECTION USING RING BEAM SYSTEM M. Hiaki, K. Takamasu and S. Ozono Depatment of Peision Engineeing, The Univesity of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo, Japan Abstat: In this pape, we popose

More information

Review of Vector Algebra and Vector Calculus Operations

Review of Vector Algebra and Vector Calculus Operations Revew of Vecto Algeba and Vecto Calculus Opeatons Tpes of vaables n Flud Mechancs Repesentaton of vectos Dffeent coodnate sstems Base vecto elatons Scala and vecto poducts Stess Newton s law of vscost

More information

Remember: When an object falls due to gravity its potential energy decreases.

Remember: When an object falls due to gravity its potential energy decreases. Chapte 5: lectc Potental As mentoned seveal tmes dung the uate Newton s law o gavty and Coulomb s law ae dentcal n the mathematcal om. So, most thngs that ae tue o gavty ae also tue o electostatcs! Hee

More information

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o? Test 1 phy 0 1. a) What s the pupose of measuement? b) Wte all fou condtons, whch must be satsfed by a scala poduct. (Use dffeent symbols to dstngush opeatons on ectos fom opeatons on numbes.) c) What

More information

Stereo Matching Using Fusion of Spatial Weight Variable Window and Adaptive Support Weight

Stereo Matching Using Fusion of Spatial Weight Variable Window and Adaptive Support Weight Intenatonal Jounal of Compute an Eletal Engneeng, Vol. 6, No. 3, June 2014 Steeo Mathng Usng Fuson of Spatal Weght Vaable Wnow an Aaptve Suppot Weght Phu Nguyen Hong an Chang Woo Ahn ost. Some popula methos

More information

Dynamics of social networks (the rise and fall of a networked society)

Dynamics of social networks (the rise and fall of a networked society) Dynams of soal networks (the rse and fall of a networked soety Matteo Marsl, ICTP Treste Frantsek Slanna, Prague, Fernando Vega-Redondo, Alante Motvaton & Bakground Soal nteraton and nformaton Smple model

More information

PHYSICS 212 MIDTERM II 19 February 2003

PHYSICS 212 MIDTERM II 19 February 2003 PHYSICS 1 MIDERM II 19 Feruary 003 Exam s losed ook, losed notes. Use only your formula sheet. Wrte all work and answers n exam ooklets. he aks of pages wll not e graded unless you so request on the front

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding

More information

Khintchine-Type Inequalities and Their Applications in Optimization

Khintchine-Type Inequalities and Their Applications in Optimization Khntchne-Type Inequaltes and The Applcatons n Optmzaton Anthony Man-Cho So Depatment of Systems Engneeng & Engneeng Management The Chnese Unvesty of Hong Kong ISDS-Kolloquum Unvestaet Wen 29 June 2009

More information

Analytic Framework for Blended Multiple Model Systems Using Linear Local Models. D.J. Leith W.E. Leithead

Analytic Framework for Blended Multiple Model Systems Using Linear Local Models. D.J. Leith W.E. Leithead Analyt Fameok fo Blended Multple Model Systems Usng nea oal Models D.J. eth W.E. ethead Depatment of Eletons & Eletal Engneeng, Unvesty of Stathlyde, 5 Geoge St., Glasgo G QE Tel. +44 4 548 47, Fa: +44

More information

Interpolation-based Parametric Model Reduction using Krylov Subspaces

Interpolation-based Parametric Model Reduction using Krylov Subspaces Inteolaton-ased Paamet Model Reduton usng Kylov Susaes Rudy Ed, Bos Lohmann and Heko Panze utumn Shool on Futue Develoments n MOR, eshellng. Seteme 009 Outlne Motvaton Shot ovevew of the exstng methods

More information

Design of Petri Net-based Deadlock Prevention Controllers for Flexible Manufacturing Systems

Design of Petri Net-based Deadlock Prevention Controllers for Flexible Manufacturing Systems Poeedngs of te 2009 IEEE Intenatonal Confeene on Systems, an, and Cybenets San Antono, TX, USA - Otobe 2009 Desgn of Pet Net-based Deadlo Peventon Contolles fo Flexble anufatung Systems Guoqang Zeng, Wemn

More information

Tian Zheng Department of Statistics Columbia University

Tian Zheng Department of Statistics Columbia University Haplotype Tansmsson Assocaton (HTA) An "Impotance" Measue fo Selectng Genetc Makes Tan Zheng Depatment of Statstcs Columba Unvesty Ths s a jont wok wth Pofesso Shaw-Hwa Lo n the Depatment of Statstcs at

More information

Chapter 8. Linear Momentum, Impulse, and Collisions

Chapter 8. Linear Momentum, Impulse, and Collisions Chapte 8 Lnea oentu, Ipulse, and Collsons 8. Lnea oentu and Ipulse The lnea oentu p of a patcle of ass ovng wth velocty v s defned as: p " v ote that p s a vecto that ponts n the sae decton as the velocty

More information

Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0

Suppose you have a bank account that earns interest at rate r, and you have made an initial deposit of X 0 IOECONOMIC MODEL OF A FISHERY (ontinued) Dynami Maximum Eonomi Yield In ou deivation of maximum eonomi yield (MEY) we examined a system at equilibium and ou analysis made no distintion between pofits in

More information

BINARY LAMBDA-SET FUNCTION AND RELIABILITY OF AIRLINE

BINARY LAMBDA-SET FUNCTION AND RELIABILITY OF AIRLINE BINARY LAMBDA-SET FUNTION AND RELIABILITY OF AIRLINE Y. Paramonov, S. Tretyakov, M. Hauka Ra Tehnal Unversty, Aeronautal Insttute, Ra, Latva e-mal: yur.paramonov@mal.om serejs.tretjakovs@mal.om mars.hauka@mal.om

More information

Approximate Abundance Histograms and Their Use for Genome Size Estimation

Approximate Abundance Histograms and Their Use for Genome Size Estimation J. Hlaváčová (Ed.): ITAT 2017 Poceedngs, pp. 27 34 CEUR Wokshop Poceedngs Vol. 1885, ISSN 1613-0073, c 2017 M. Lpovský, T. Vnař, B. Bejová Appoxmate Abundance Hstogams and The Use fo Genome Sze Estmaton

More information

Multi-Objective Optimization Algorithms for Finite Element Model Updating

Multi-Objective Optimization Algorithms for Finite Element Model Updating Multi-Objective Optimization Algoithms fo Finite Element Model Updating E. Ntotsios, C. Papadimitiou Univesity of Thessaly Geece Outline STRUCTURAL IDENTIFICATION USING MEASURED MODAL DATA Weighted Modal

More information

State Estimation. Ali Abur Northeastern University, USA. Nov. 01, 2017 Fall 2017 CURENT Course Lecture Notes

State Estimation. Ali Abur Northeastern University, USA. Nov. 01, 2017 Fall 2017 CURENT Course Lecture Notes State Estmaton Al Abu Notheasten Unvesty, USA Nov. 0, 07 Fall 07 CURENT Couse Lectue Notes Opeatng States of a Powe System Al Abu NORMAL STATE SECURE o INSECURE RESTORATIVE STATE EMERGENCY STATE PARTIAL

More information

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid:

Non-Ideal Gas Behavior P.V.T Relationships for Liquid and Solid: hemodynamis Non-Ideal Gas Behavio.. Relationships fo Liquid and Solid: An equation of state may be solved fo any one of the thee quantities, o as a funtion of the othe two. If is onsideed a funtion of

More information

The virial theorem and the kinetic energy of particles of a macroscopic system in the general field concept

The virial theorem and the kinetic energy of particles of a macroscopic system in the general field concept Contnuum Mehans and Themodynams, Vol. 9, Issue, pp. 61-71 (16). https://dx.do.og/1.17/s161-16-56-8. The al theoem and the knet enegy of patles of a maosop system n the geneal feld onept Segey G. Fedosn

More information

Lecture 26 Finite Differences and Boundary Value Problems

Lecture 26 Finite Differences and Boundary Value Problems 4//3 Leture 6 Fnte erenes and Boundar Value Problems Numeral derentaton A nte derene s an appromaton o a dervatve - eample erved rom Talor seres 3 O! Negletng all terms ger tan rst order O O Tat s te orward

More information

( ) F α. a. Sketch! r as a function of r for fixed θ. For the sketch, assume that θ is roughly the same ( )

( ) F α. a. Sketch! r as a function of r for fixed θ. For the sketch, assume that θ is roughly the same ( ) . An acoustic a eflecting off a wav bounda (such as the sea suface) will see onl that pat of the bounda inclined towad the a. Conside a a with inclination to the hoizontal θ (whee θ is necessail positive,

More information

Bayesian Analysis of Topp-Leone Distribution under Different Loss Functions and Different Priors

Bayesian Analysis of Topp-Leone Distribution under Different Loss Functions and Different Priors J. tat. Appl. Po. Lett. 3, No. 3, 9-8 (6) 9 http://dx.doi.og/.8576/jsapl/33 Bayesian Analysis of Topp-Leone Distibution unde Diffeent Loss Functions and Diffeent Pios Hummaa ultan * and. P. Ahmad Depatment

More information

CEEP-BIT WORKING PAPER SERIES. Efficiency evaluation of multistage supply chain with data envelopment analysis models

CEEP-BIT WORKING PAPER SERIES. Efficiency evaluation of multistage supply chain with data envelopment analysis models CEEP-BIT WORKING PPER SERIES Effcency evaluaton of multstage supply chan wth data envelopment analyss models Ke Wang Wokng Pape 48 http://ceep.bt.edu.cn/englsh/publcatons/wp/ndex.htm Cente fo Enegy and

More information

(conservation of momentum)

(conservation of momentum) Dynamis of Binay Collisions Assumptions fo elasti ollisions: a) Eletially neutal moleules fo whih the foe between moleules depends only on the distane between thei entes. b) No intehange between tanslational

More information

Chapter Eight Notes N P U1C8S4-6

Chapter Eight Notes N P U1C8S4-6 Chapte Eight Notes N P UC8S-6 Name Peiod Section 8.: Tigonometic Identities An identit is, b definition, an equation that is alwas tue thoughout its domain. B tue thoughout its domain, that is to sa that

More information